Overcoming Performance Losses in Scaling-up Metal Oxide-based Solar Water Splitting Devices
Ibbi Y. Ahmet a, Yimeng Ma a, Ronald R. Gutierrez b, Roel van de Krol a, Sophia Haussener b, Fatwa F. Abdi a
a Helmholtz-Zentrum Berlin für Materialien und Energie GmbH, Germany, Berlin, Germany
b Laboratory of Renewable Energy Science and Engineering, École Polytechnique Fédérale de Lausanne, Switzerland
Materials for Sustainable Development Conference (MATSUS)
Proceedings of nanoGe Fall Meeting19 (NFM19)
#SolFuel19. Solar Fuel Synthesis: From Bio-inspired Catalysis to Devices
Berlin, Germany, 2019 November 3rd - 8th
Organizers: Roel van de Krol and Erwin Reisner
Oral, Fatwa F. Abdi, presentation 141
DOI: https://doi.org/10.29363/nanoge.nfm.2019.141
Publication date: 18th July 2019

Progress in the development of metal oxide photoelectrodes in the past 10-15 years has shifted focus towards fabricating practical stand-alone solar water splitting devices. Integrated tandem devices in near-neutral pH electrolytes based on the combination of a BiVO4-based photoanode as a wide-bandgap top absorber and various types of bottom absorbers have been reported, and solar-to-hydrogen (STH) efficiencies approaching 10% have been demonstrated.[1-2] Nevertheless, the majority of these demonstration devices still have active areas of less than 1 cm2. The next step is to move beyond lab-scale experiments and demonstrate large-area devices. Here, we report the scale-up of spray-deposited BiVO4 photoanodes from <1 to 50 cm2, from which we observed a significant performance loss with increased area. An unbiased 50 cm2 PV-PEC water splitting device is demonstrated with an STH efficiency of 2.1%. While this is the highest reported value for a large-area (> 10 cm2) BiVO4-based water splitting device, it is still a factor of 2-3 lower than the efficiency achieved using the corresponding small-area device. By performing a series of control experiments, we found that factors other than the BiVO4 itself, such as substrate conductivity, electrolyte conductivity, and cell geometry, are responsible for a total voltage loss of 600 mV and therefore limit the performance of the large-area photoanode. The different loss mechanisms associated with scaling-up photoelectrodes were further quantified using a finite element analysis model (COMSOL Multiphysics®). Based on these insights, electrochemical engineering strategies to overcome these losses are offered, which would limit the voltage loss for large-area photoelectrodes to less than 50 mV.

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